What is the Role of Matter in General Relativity's Lagrangian?

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Discussion Overview

The discussion revolves around the role of matter in the context of the Lagrangian formulation of General Relativity (GR), specifically focusing on how matter is defined within the Einstein-Hilbert action and its implications for various types of particles, including massless particles and gravitons.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the definition of the Lagrangian for matter fields in GR, seeking clarity on what constitutes matter in this context.
  • Another participant asserts that in the GR Lagrangian, matter is defined as anything that is not spacetime geometry, including terms like the Ricci scalar and metric determinant.
  • A subsequent inquiry asks whether massless particles fall under the definition of matter, to which some participants respond affirmatively, clarifying that massless particles other than gravitons are included.
  • There is a discussion about gravitons, with a participant noting that they would be described by the part of the Lagrangian involving only the metric and its derivatives, and thus are not considered matter in the same sense.
  • Concerns are raised regarding the current understanding and quantization of the gravitational field, indicating that a satisfactory description of gravitons remains elusive.
  • Another participant references notes on massive gravity, distinguishing it from the standard concept of massless gravitons.

Areas of Agreement / Disagreement

Participants generally agree that matter in the context of the GR Lagrangian includes massless particles other than gravitons. However, there is no consensus on the satisfactory description of gravitons or their role in the Lagrangian, indicating ongoing debate and uncertainty.

Contextual Notes

The discussion highlights limitations in the current understanding of gravitons and their quantization, as well as the potential confusion between massive gravity and the concept of massless gravitons.

dsaun777
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I was going over the Einstein-Hilbert action derivation of the Einstein field equations and came across a term that does not seem to be explicitly defined. That term is the Langragian for the matter fields. What exactly is matter in General relativity in the context of the Lagrangian? Here is one equation with the subscript "matter."
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In the GR Lagrangian, matter is anything that isn't spacetime geometry; i.e., anything that isn't the Ricci scalar or the metric determinant (or the cosmological constant if that term is included).
 
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PeterDonis said:
In the GR Lagrangian, matter is anything that isn't spacetime geometry; i.e., anything that isn't the Ricci scalar or the metric determinant (or the cosmological constant if that term is included).
Would that include massless particles?
 
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dsaun777 said:
Would that include massless particles?

As long as they aren't gravitons, yes.
 
dsaun777 said:
Would that include massless particles?
Yes. Or, for instance, an electromagnetic field. Not mass, but energy-momentum sources gravity.
 
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PeterDonis said:
As long as they aren't gravitons, yes.
The gravitons would be described by the part of the Lagrangian involving only the metric and its derivatives. In standard GR it's
$$\mathcal{L}=\sqrt{-g} R.$$
This includes also interaction terms of the gravitons, as to be expected from a non-Abelian gauge theory. Gravitons as particles would be defined as the asymptotic free states.

The only trouble is that this doesn't work out as it does for the other interactions, and that's why the quantization of the gravitational field is not yet brought into a satisfactory state :-(.
 
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vanhees71 said:
The gravitons would be described by the part of the Lagrangian involving only the metric and its derivatives.

Yes, that's why I said, in response to the OP, that "matter" includes massless particles other than gravitons, but not gravitons.
 
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vanhees71 said:
The gravitons would be described by the part of the Lagrangian involving only the metric and its derivatives. In standard GR it's
$$\mathcal{L}=\sqrt{-g} R.$$
This includes also interaction terms of the gravitons, as to be expected from a non-Abelian gauge theory. Gravitons as particles would be defined as the asymptotic free states.

The only trouble is that this doesn't work out as it does for the other interactions, and that's why the quantization of the gravitational field is not yet brought into a satisfactory state :-(.
?
Do you know of any relatively light, no pun intended, material about gravitons?
 
No. The problem is nobody has found a satisfactory description of gravitons yet.
 
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dsaun777 said:
?
Do you know of any relatively light, no pun intended, material about gravitons?
These notes of Hinterbichler about massive gravity,

https://arxiv.org/abs/1105.3735

are great imo.
 
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  • #11
haushofer said:
massive gravity

Note that, as the introduction of the notes you reference explains, massive gravity is not the same as the standard concept of "gravitons", i.e., massless spin-2 particles.
 
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